US3157124A - Spin stabilized hollow charge projectile - Google Patents

Spin stabilized hollow charge projectile Download PDF

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Publication number
US3157124A
US3157124A US164001A US16400162A US3157124A US 3157124 A US3157124 A US 3157124A US 164001 A US164001 A US 164001A US 16400162 A US16400162 A US 16400162A US 3157124 A US3157124 A US 3157124A
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Prior art keywords
projectile
charge
insert
spin
hollow
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Expired - Lifetime
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US164001A
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Muller Helmut
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Rheinmetall Industrie AG
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Rheinmetall GmbH
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F42AMMUNITION; BLASTING
    • F42BEXPLOSIVE CHARGES, e.g. FOR BLASTING, FIREWORKS, AMMUNITION
    • F42B12/00Projectiles, missiles or mines characterised by the warhead, the intended effect, or the material
    • F42B12/02Projectiles, missiles or mines characterised by the warhead, the intended effect, or the material characterised by the warhead or the intended effect
    • F42B12/04Projectiles, missiles or mines characterised by the warhead, the intended effect, or the material characterised by the warhead or the intended effect of armour-piercing type
    • F42B12/10Projectiles, missiles or mines characterised by the warhead, the intended effect, or the material characterised by the warhead or the intended effect of armour-piercing type with shaped or hollow charge
    • F42B12/12Projectiles, missiles or mines characterised by the warhead, the intended effect, or the material characterised by the warhead or the intended effect of armour-piercing type with shaped or hollow charge rotatably mounted with respect to missile housing

Definitions

  • the present invention relates to a spin-stabilized hollow-charge projectile, consisting as usual of a body with an explosive charge and a detonator and also an insert.
  • the object of the present invention is to reduce or completely eliminate this loss of power in spin-stabilized hollow-charge projectiles.
  • the hollow-charge projectile according to the invention which likewise comprises a section rotatably mounted in the interior of the projectile body and driving means therefor.
  • a characteristic feature of the type of construction according to the invention is that the rotatably mounted parts of the projectile consist only of the insert connected to the driving means and designed as a coaxial body of revolution.
  • the hollow-charge projectile according to the invention is based on two new discoveries connected with explosion engineering.
  • the malfunctioning of a strongly rotating hollow charge is due especially to the rotation of the insert mass and only to a very small extent to the rotation of the explosive.
  • the explosive charge must not rest absolutely closely against the insert in order to achieve a high penetration effect, but rather there should also be a narrow circularsymmetrical gap between the insert and explosive charge. In this way, it is possible by the method according to the invention to obtain full spin compensation when the projectile reaches the target, in that precautions are taken to see that the insert is not rotating or is rotating only slowly when the projectile reaches the target, whereas the projectile body is rotating together with the explosive charge at the speed due to the spin.
  • FIG. 1 shows a hollow-charge projectile designed for the application of pressure to the driving impeller by atmospheric air
  • FIG. 2 shows a hollow-charge projectile designed for the application of pressure by powder gases and by atmospheric air.
  • the hollow-charge projectile according to FIG. 1 has an insert 1 which is fixedly connected to the driving impeller Z; the two parts can rotate together with respect to the projectile body 3 and the explosive charge 4.
  • An antifriction bearing 5 is arranged in the supporting member '7 fixedly connected to the nose 6 of the projectile body 3, while a plain pivot bearing #8 is let into the explosive charge 4. Said bearing rests on a spring 9 which yields on firing until the gap 10, which separates the insert 1 from the explosive charge 4, is closed.
  • the gap 10 can be filled with a liquid of low viscosity.
  • a high liquid pressure is then produced for a short time in the gap 10.
  • the volume of liquid can either be kept constant in the gap 10 on firing or part of the liquid can be forced through the labyrinth packing 14; in the last-mentioned case, the planned width of the gap 10 is restored only when the acceleration of the projectile abates, in accordance with the dimensioning of the spring 9 and the load applied to the driving impeller 2 by thedynamic air pressure during the in the gap 10 which have been described, only a very slight rotation which is not harmful to the hollow-charge effect is imparted to the insert l on firing owing to the liquid friction and theiadditional bearing frictiong-this rotation being compensated in a very short -time bya particularly lightlyconstructed driving'impeller '2, so that, even-for
  • FIG. 2 shows "a hollow charge projectilewith an advan tageous design of the driving impeller 2;
  • the air accumuiated ordammednpduringtheflight ofthe projectile is fedfcentrallyito the .driving impeller 2 through an air duct 'coaxialuwithIsaidprojectile and the connected ducts116," so that: thetul'l ramspressure is utilised for said impeller
  • a hollow space 17 in which, in addition, there canrbe accommodated: a powder propelling composition which is advantageouslyiignited-immediatelyas the projectile leaves the barrel.
  • the .powder gases escape throughithe bores:
  • impeller 2 substantially morestrongly: than it is possible for the dynamic air-pressure to do. With this arrangement, even without providingthe above-describedsliquid cushion, theispeedof the.
  • hollow-chargeprojectiles described abovewith reference to FIGS.I1 and1'2 merely'irepresent embodiments of the present-inventionuwhich:is by no means limited thereto; but covers in principle all hollow-charge projec-' tiles provided with' al more or less marked spin compensationof the insert;
  • Method-of increasing" the penetrating power of a hollow-charge projectile stabilized in flight by spin comprising rotating the projectile body together with the explos'ivecharge at a speeddependent on thespin at least on reaching the target, and rotating the insert in the opposite'direction to the point of approximate compensation"- of the movement due to the spin.

Description

Nov. 17, 1964 H. MULLER 3,157,124
SPIN STABILIZED HOLLOW CHARGE PROJECTILE Filed Jan. '5, 1962 2 Sheets-Sheet l Jnvemar:
ZL eh y m ,GMZQ M t, m
Nov. 17, 1964 H. MULLER 3,157,124
SPIN STABILIZED HOLLOW CHARGE PROJECTILE Filed Jan. 3, 1962 2 Sheets-Sheet 2 Fig. 2
Jn venfor: HeZ vwui Mb'ZZ k Attyo'.
United States Patent 3,157,124 SPIN STABILIZED HGLLGW CHARGE PRQEECTILE Helmet Miiller, Dusseldorf, Germany, assignor to Firms Rheinmetall G.m.h.H., Dusseldorf, Germany Filed Jan. 3, 1962, Ser. No. 164,001 Claims priority, application Germany, Zia 5, 19611, R 29,404 4 Claims. (Cl. lii256) The present invention relates to a spin-stabilized hollow-charge projectile, consisting as usual of a body with an explosive charge and a detonator and also an insert.
It is known that, owing to the spin of a projectile, which is indispensable for stabilizing it in fiight, a loss of power occurs on penetration of a target. The object of the present invention is to reduce or completely eliminate this loss of power in spin-stabilized hollow-charge projectiles.
Proposals for solving this problem have already become known which, however, can be carried into effect only by a particularly large expenditure in manufacturing the projectiles and postulate substantial drawbacks of another kind or only provide a partial solution. For example, it has been proposed to arrange the entire explosive portion of the projectile, that is the explosive charge with the detonator and insert, within the projectile body in a second inner jacket consisting of a casing and base for the explosive charge, connect said inner jacket fixedly to a braking turbine and mount it rotatably with respect to the projectile body in antifriction bearings. The inertia forces of this portion of the projectile, which makes up almost one half of the weight thereof, are intercepted on firing by powder gases conveyed into the interior of the projectile. An acceleration of rotation is imparted to the inner rotatably mounted portion of the projectile on firing and also during the continued flight of said projectile by the friction in the antifriction bearings, which, however, is counteracted by the braking turbine to which the pressure of the outside air dammed up during the flight of the projectile is applied. This type of construction, however, has considerable drawbacks, since a higher weight of the projectile, great complexity and high cost are unavoidable; moreover, a considerable part of the mass of the projectile does not assist in the stabilization of the latter.
Furthermore, a proposal has become known in which spin compensation is intended to be achieved by a special stepped inclined position of the operative surfaces of the insert and/ or by special provisions made in the explosive charge, with the object of producing a tangential thrust component. In this case, however, the circular symmetry of the insert and the circular-symmetrical action of the gases on the insert must be relinquished and, thereby, it is necessary to put up with disturbances which result in only partial success as regards the spin compensation.
The shortcomings of the proposals mentioned and of all other proposals which have become known are obviated by the hollow-charge projectile according to the invention which likewise comprises a section rotatably mounted in the interior of the projectile body and driving means therefor. A characteristic feature of the type of construction according to the invention is that the rotatably mounted parts of the projectile consist only of the insert connected to the driving means and designed as a coaxial body of revolution.
The hollow-charge projectile according to the invention is based on two new discoveries connected with explosion engineering. On the one hand, the malfunctioning of a strongly rotating hollow charge is due especially to the rotation of the insert mass and only to a very small extent to the rotation of the explosive. On the other hand, the explosive charge must not rest absolutely closely against the insert in order to achieve a high penetration effect, but rather there should also be a narrow circularsymmetrical gap between the insert and explosive charge. In this way, it is possible by the method according to the invention to obtain full spin compensation when the projectile reaches the target, in that precautions are taken to see that the insert is not rotating or is rotating only slowly when the projectile reaches the target, whereas the projectile body is rotating together with the explosive charge at the speed due to the spin.
Embodiments of hoflow-charge projectiles according to the invention are described hereinafter in detail With reference to the accompanying drawings, in which:
FIG. 1 shows a hollow-charge projectile designed for the application of pressure to the driving impeller by atmospheric air;
FIG. 2 shows a hollow-charge projectile designed for the application of pressure by powder gases and by atmospheric air.
The hollow-charge projectile according to FIG. 1 has an insert 1 which is fixedly connected to the driving impeller Z; the two parts can rotate together with respect to the projectile body 3 and the explosive charge 4. An antifriction bearing 5 is arranged in the supporting member '7 fixedly connected to the nose 6 of the projectile body 3, while a plain pivot bearing #8 is let into the explosive charge 4. Said bearing rests on a spring 9 which yields on firing until the gap 10, which separates the insert 1 from the explosive charge 4, is closed.
and striking against the vanes 12 of the driving impeller 2 and issuing through the ducts 13 produces a strong torque at the driving impeller 2 and thereby reduces the speed of the insert 1 fixedly connected to it to a small value in a short time, so that spin compensation is already achieved and the maximum hollowcharge ellect ensured after the shot has travelled a small distance. By means of a suitable tangential angular position of the ducts 11 and/or of the vanes 12, it is possible to produce and maintain zero speed for the insert 1, for which purpose the driving impeller 2 must supply a torque corresponding to the friction moments occurring in the rotatable parts of the projectile. Similarly, it is possible to increase the o positely directed drive of the insert 1 until; in relation to a stationary reference system, it performs a slow rotating movement in the opposite direction to the rotation of the projectile body 3 together with the explosive charge 4, in order to compensate the slight rotary impulse transmitted to the insert 1 on the detonation of the projectile by the rotating gases produced by the explosive charge 3.
For all those purposes where firing is carried out also at very short battle ranges, the gap 10 can be filled with a liquid of low viscosity. During the acceleration of the projectile in the barrel, a high liquid pressure is then produced for a short time in the gap 10. By suitable design and by dimensioning of the labyrinth packing 14, the volume of liquid can either be kept constant in the gap 10 on firing or part of the liquid can be forced through the labyrinth packing 14; in the last-mentioned case, the planned width of the gap 10 is restored only when the acceleration of the projectile abates, in accordance with the dimensioning of the spring 9 and the load applied to the driving impeller 2 by thedynamic air pressure during the in the gap 10 which have been described, only a very slight rotation which is not harmful to the hollow-charge effect is imparted to the insert l on firing owing to the liquid friction and theiadditional bearing frictiong-this rotation being compensated in a very short -time bya particularly lightlyconstructed driving'impeller '2, so that, even-for the ple--'100 metres,theinserthas zero speed with 'respectto a stationary reference system: or a'small'speed in theopp'osite direction to thei'spin'and retains :this speed during'the further flight f 1 the" projectile.
shortestbattle range which may be concerned;for exam- 1,
FIG. 2 shows "a hollow charge projectilewith an advan tageous design of the driving impeller 2; The air accumuiated ordammednpduringtheflight ofthe projectile is fedfcentrallyito the .driving impeller 2 through an air duct 'coaxialuwithIsaidprojectile and the connected ducts116," so that: thetul'l ramspressure is utilised for said impeller In the nose .6 of the projectile there is provided a hollow space 17 in which, in addition, there canrbe accommodated: a powder propelling composition which is advantageouslyiignited-immediatelyas the projectile leaves the barrel. The .powder gases escape throughithe bores:
18 tandzimpingeionthe'r'driving: impeller 2 substantially morestrongly: than it is possible for the dynamic air-pressure to do. With this arrangement, even without providingthe above-describedsliquid cushion, theispeedof the.
inserttl canalreadyihave dropped to such an extent at a battle range .of a few hundred metres that an unreduced hollow-charge effect is obtained.
Thethollowecharge projec'tiles'according to the inventionzare of simple construction; the additional. weight em ployedias comparedewithxa similar hollow-charge projec-" tileain whichithere: is no; spin compensation is only a few percentzof thexweightethereofr Likewise, the reduction of the explosive charge :due to theigapzbetween the insertand saidiexplosive charge .is extremely small; Important also is the. fact that,:intspite'-of the:spin:compensation, there is practically? no loss ofstability in flight a'ndtno worseningof the position of thecentre-ofgravity as compared with a hollow-charge projectile-without"spin compensation,-
since onlyr spin compensation :of the insert-takes place.
The hollow-chargeprojectiles described abovewith reference to FIGS.I1 and1'2 merely'irepresent embodiments of the present-inventionuwhich:is by no means limited thereto; but covers in principle all hollow-charge projec-' tiles provided with' al more or less marked spin compensationof the insert;
What: "Iclaim is: r
- 1. Method-of increasing" the penetrating power of a hollow-charge projectile stabilized in flight by spin, comprising rotating the projectile body together with the explos'ivecharge at a speeddependent on thespin at least on reaching the target, and rotating the insert in the opposite'direction to the point of approximate compensation"- of the movement due to the spin.
2. Method according to claiin 1, characterized in that the drive of the insert in the opposite direction is increased until it follows a rotating'movement in the opposite direotion to the'spin in relation to a stationary reference system.
3. Spin-stabilized hollow-charge projectile with stabilized penetrating power comprisinga body having an explosive charge with-a detonator therein, an insert in the body, driving means connectedto the insert mounted rotatably in the interior of the body to obtain a rotary move- 'ment of the insert in the projectile in the direction opposite to thespin thereof, the ins ert connected to thedriving means :forming a coaxial body :of revolution, and the a a, outer surface of the insert forms together with the surface of a corresponding cavity in the explosive charge anar'row gap which renders possible contact-free rotation of the insert with respect to the eXpl'osive'charge restingfixe'dly' in the projectile body.
4. "Spimstabilized hollow-charge projectile-with stabilized penetrating power comprising a body having anex- 1 plosive charge Witha detonator'therein, an insert in the body,'driving means connected-to the insert mounted rotatably in the interior-of thebody to obtain a rotarymovement'of the insert in the projectile in the directionopposite to the spin thereof, the insertconnected'to the driving means forming a coaxial body 'ofravolution, the driving means is in the form of an impeller on the insert as a tur-" bine impeller to provide theapplication of pressure during theiflight of the-projectile bya stream of air='conducted through the interior of the body, said nose of the projectile having'a powder composition therein, wherebythe' gases from the powder propelling: composition "will drive the OTHER REFERENCES German application R 29404 Ic/72d,filed I an. 5, 19611 BENJAMIN A; BORCHELT, Primary Examiner. SAMUEL BOYD, Examiner.

Claims (1)

1. METHOD OF INCREASING THE PENETRATING POWER OF A HOLLOW-CHARGE PROJECTILE STABILIZED IN FLIGHT BY SPIN, COMPRISING ROTATING THE PROJECTILE BODY TOGETHER WITH THE EXPLOSIVE CHARGE AT A SPEED DEPENDENT ON THE SPIN AT LEAST
US164001A 1961-01-05 1962-01-03 Spin stabilized hollow charge projectile Expired - Lifetime US3157124A (en)

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DER29404A DE1137351B (en) 1961-01-05 1961-01-05 Twist-stabilized shaped charge projectile

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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3302567A (en) * 1964-03-09 1967-02-07 Dresser Ind Shaped-charge booster
US3439613A (en) * 1964-11-26 1969-04-22 Bolkow Gmbh Self-propelled hollow charge having concave liner with propellant contained therein
US4102271A (en) * 1976-02-12 1978-07-25 Rheinmetall Gmbh. Armor-piercing tandem shell or projectile
US4982665A (en) * 1973-11-29 1991-01-08 The United States Of America As Represented By The Secretary Of The Navy Shaped charge
US5194690A (en) * 1990-02-21 1993-03-16 Teledyne Industries, Inc. Shock compression jet gun
US5235916A (en) * 1966-01-10 1993-08-17 Hughes Missile Systems Company Warhead directed-charge positioner system
EP2487451A3 (en) * 2011-02-10 2015-04-29 TDW Gesellschaft für verteidigungstechnische Wirksysteme mbH Hollow charge penetrator
US10215543B1 (en) * 2012-05-10 2019-02-26 Mark Benson Linear explosive disruptor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB8719846D0 (en) * 1987-08-21 1987-09-30 Ici Plc Shaped primer

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
BE564801A (en) * 1957-02-19
US2623465A (en) * 1949-02-15 1952-12-30 Brandt Soc Nouv Ets Projectile
US2787958A (en) * 1952-09-15 1957-04-09 Belge De Mecanique Et D Armeme Projectile
US2900873A (en) * 1955-11-10 1959-08-25 Haut Rhin Manufacture Machines Ordnance
US2981188A (en) * 1955-10-10 1961-04-25 Henry S Lipinski Spin-stabilized projectile with nonrotating shaped charge

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2623465A (en) * 1949-02-15 1952-12-30 Brandt Soc Nouv Ets Projectile
US2787958A (en) * 1952-09-15 1957-04-09 Belge De Mecanique Et D Armeme Projectile
US2981188A (en) * 1955-10-10 1961-04-25 Henry S Lipinski Spin-stabilized projectile with nonrotating shaped charge
US2900873A (en) * 1955-11-10 1959-08-25 Haut Rhin Manufacture Machines Ordnance
BE564801A (en) * 1957-02-19
GB886225A (en) * 1957-02-19 1962-01-03 Rheinmetall Gmbh Improvements in and relating to spin-stabilised hollow charge projectiles

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3302567A (en) * 1964-03-09 1967-02-07 Dresser Ind Shaped-charge booster
US3439613A (en) * 1964-11-26 1969-04-22 Bolkow Gmbh Self-propelled hollow charge having concave liner with propellant contained therein
US5235916A (en) * 1966-01-10 1993-08-17 Hughes Missile Systems Company Warhead directed-charge positioner system
US4982665A (en) * 1973-11-29 1991-01-08 The United States Of America As Represented By The Secretary Of The Navy Shaped charge
US4102271A (en) * 1976-02-12 1978-07-25 Rheinmetall Gmbh. Armor-piercing tandem shell or projectile
US5194690A (en) * 1990-02-21 1993-03-16 Teledyne Industries, Inc. Shock compression jet gun
US5303633A (en) * 1990-02-21 1994-04-19 Teledyne Industries, Inc. Shock compression jet gun
EP2487451A3 (en) * 2011-02-10 2015-04-29 TDW Gesellschaft für verteidigungstechnische Wirksysteme mbH Hollow charge penetrator
US10215543B1 (en) * 2012-05-10 2019-02-26 Mark Benson Linear explosive disruptor

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DE1137351B (en) 1962-09-27
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